Existence and Global Attractivity of Positive Periodic Solutions for The Neutral Multidelay Logarithmic Population Model with Impulse
Abstract
Suffiicient and realistic conditions are established in this paper for the existence and global attractivity of a positive periodic solution to the neutral multidelay logarithmic population model with impulse by using the theory of abstract continuous theorem of k-set contractive operator and some inequality techniques. The results improve and generalize the known ones in Li 1999, Lu and Ge 2004, Y. Luo and Z. G. Luo 2010, and Wang et al. 2009. As an application, we also give an example to illustrate the feasibility of our main results.
1. Introduction
On the other hand, there are some other perturbations in the real world such as fires and floods, which are not suitable to be considered continually. These perturbations bring sudden changes to the system. Systems with such sudden perturbations involving impulsive differential equations have attracted the interest of many researchers in the past twenty years [13–19], since they provide a natural description of several real processes subject to certain perturbations whose duration is negligible in comparison with the duration of the process. Such processes are often investigated in various fields of science and technology such as physics, population dynamics, ecology, biological systems, and optimal control. For details, see [20–22].
However, to this day, no scholars had done works on the existence, uniqueness, and global stability of the positive periodic solution of (1). One could easily see that the systems (5)–(7) are all special cases of the system (1). Therefore, we propose and study the system (1) in this paper.
Throughout this paper, we make the following notations.
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Cω = {x∣x ∈ C(R, R), x(t + ω) = x(t)}, with the norm defined by |x|0 = max t∈[0,ω] | x(t)|,
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, with the norm defined by ∥x∥ = max t∈[0,ω]{|x|0, |x′|0}.
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(H1) r(t), a(t), bi(t), cj(t), dl(t), σi(t), τl(t) (i = 1,2, …, n; j = 1,2, …, m; l = 1,2, …, p) are all positive periodic continuous functions with period ω > 0;
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(H2) 0 < t1 < t2 < ⋯<tk < ⋯ are fixed impulsive points with limk→∞tk = +∞;
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(H3) {θk} is a real sequence such that θk + 1 > 0, and is an ω-periodic function.
In the following section, some definitions and some useful lemmas are listed. In the third section, by using an abstract continuous theorem of k-set contractive operator and some inequality techniques, we acquired some sufficient conditions which ensure the existence and uniqueness of the positive periodic solution of the systems (1) and (2). Finally, we give an example to show our results.
2. Preliminaries
In order to obtain the existence and uniqueness of a periodic solution for the systems (1) and (2), we first give some definitions and lemmas.
Definition 1 (see [21].)A function N : R → (0, +∞) is said to be a positive solution of (1) and (2), if the following conditions are satisfied:
Definition 2. The system (1) is said to be globally attractive, if there exists a positive solution x(t) of (1) such that lim t→+∞ | x(t) − y(t)| = 0 for any other positive solution y(t) of (1).
We can easily get the following Lemma 3.
Lemma 3. The region R = {N(t) : N(0) > 0, t ≥ 0} is invariant with respect to (1).
Proof. In view of biological population, we obtain N(0) > 0. By the system (1), we have
Under the above hypotheses (H1)–(H3), we consider the following neutral nonimpulsive system:
The following lemmas will be used in the proofs of our results, and the proof of the lemma is similar to that of Theorem 1 in [13].
Lemma 4. Suppose that (H1)–(H4) hold. Then,
Proof. (1) It is easy to see that is absolutely continuous on every interval (tk, tk+1], t ≠ tk, k = 1,2, …,
(2) Since is absolutely continuous on every interval (tk, tk+1], t ≠ tk, k = 1,2, …, and in view of (15), it follows that for any k = 1,2, …,
Definition 5 (see [23].)Let U be a bounded subset in X. Define that
Definition 6 (see [23].)Let X, Y be two Banach spaces and D ⊂ X; a continuous and bounded map T : D → Y is called k-set contractive if for any bounded set U ⊂ D one has
For a Fredholm operator L : X → Y with index zero, according to [9, 24], we define
Lemma 7 (see [9], [24].)Let L : X → Y be a Fredholm operator with zero index and a ∈ Y be a fixed point. Suppose that N : Ω → Y is called a k-set contractive with k < l(L), where Ω ⊂ X is bounded, open, and symmetric about 0 ∈ Ω. Further, one also assumes that
- (1)
Lx ≠ λNx + λa, for x ∈ ∂Ω, λ ∈ (0,1);
- (2)
[QN(x) + Qa, x] [QN(−x) + Qa, x] < 0, for x ∈ Ker L⋂ ∂Ω;
where [·, ·] is a bilinear form on Y × X and Q is the projection of Y onto Coker(L), where Coker(L) is the cokernel of the operator L. Then, there is an such that Lx − Nx = a.
Lemma 8 (see [25].)The differential operator L is a Fredholm operator with index zero and satisfies l(L) ≥ 1.
Lemma 9. Let r0, r1 be two positive constants and . If , then is a k-set contractive map.
As Lemma 9 can be proved in the same way as in the proof of Lemma 2.4 in [7], we omit it here.
Lemma 10 (see [7], [9].)Suppose that and τ′(t) < 1, t ∈ [0, ω], then the function t − τ(t) has a unique inverse μ(t) satisfying μ ∈ C(R, R) with μ(a + ω) = μ(a) + ω for all a ∈ R, and if g ∈ PCω, τ′(t) < 1, t ∈ [0, ω], then g(μ(t)) ∈ PCω.
Suppose that x(t) is a differently continuous ω-periodic function on R with (ω > 0), then to any .
3. Main Theorem
Remark 12. From Lemma 9, we get that ζi(ω) = ζi(0) + ω, ξl(ω) = ξl(0) + ω, i = 1,2, …, n; l = 1,2, …, p; then,
Theorem 13. In addition to (H1)–(H3), suppose that the following conditions hold:
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(H4) there exists a constant η > 0 such that |Γ(t)| ≥ η, for all t ∈ [0, ω], where Γ(t) is defined by (23);
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(H5) if , and .
Then, (1) has at least one positive ω-periodic solution.
Proof. Let u(t) be an arbitrary ω-periodic solution of the operator equation as follows:
Since , for all l = 1,2, …, p, it follows that . So from Theorem 13, we have the following result.
Corollary 14. Suppose that (H1)–(H3) and the following conditions hold:
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there exists a constant η > 0 such that |Γ(t)| ≥ η, for all t ∈ [0, ω], where Γ(t) is defined by (23);
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if .
Then (1) has at least one positive ω-periodic solution.
On the other hand, if , for all l = 1,2, …, p, it follows that . So from Theorem 13, we also have the following result.
Corollary 15. Suppose that (H1)–(H3) and the following conditions hold:
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there exists a constant η > 0 such that |Γ(t)| ≥ η, for all t ∈ [0, ω], where Γ(t) is defined by (23);
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if .
Then, (1) has at least one positive ω-periodic solution.
Our next theorem is concerned with the global attractivity of periodic solution of the system (1).
Theorem 16. Suppose that (H1)–(H5) and the following conditions hold:
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(H6) there is a positive constant μ such that
() -
(H7) , as t → +∞.
Then, the positive ω-periodic solution of (1) is globally attractive, where .
Proof. Suppose that y(t) = ev(t) is a positive ω-periodic solution of (10), is another positive solution of (10). Similar to (17), we have
Corollary 17. Suppose that the following conditions hold:
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r(t), a(t), bi(t), cj(t), dl(t), σi(t), τl(t) (i = 1,2, …, n; j = 1,2, …, m; l = 1,2, …, p) are all positive ω-periodic continuous functions with σi(t) ≥ 0, τl(t) ≥ 0, t ∈ [0, ω], , , for all i = {1,2, …, n}, for all l = {1,2, …, p}; furthermore, dl(t) ∈ C1(R, R), , for all j = {1,2, …, m}, for all l = {1,2, …, p};
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there exists a constant η > 0 such that |Γ*(t)| ≥ η, for all t ∈ [0, ω], where Γ*(t) is defined by the following:
() -
if , and .
Then, (61) has at least one positive ω-periodic solution.
Corollary 18. Suppose that and the following conditions hold:
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there is a positive constant μ such that
() -
, as t → +∞.
Then, the positive ω-periodic solution of (61) is globally attractive, where .
4. An Example
Corollary 20. Suppose that (H1)–(H3) and the following conditions hold:
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(H4) there exists a constant η > 0 such that |Γ(t)| ≥ η, for all t ∈ [0, ω], where Γ(t) is defined by the following:
() -
(H5) if , and |1 − τ′|0 | D|0 < 1.
Then, (64) has at least one positive ω-periodic solution, where
Corollary 21. Suppose that (H1)–(H5) and the following conditions hold:
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(H6) there is a positive constant μ such that
() -
(H7) , as t → +∞.
Then, the positive ω-periodic solution of (64) is globally attractive, where H(t): = [D′(t) + D(t)A(t)] [1 − τ′(t)] + D(t)τ′′(t)/[1 − τ′(t)] 2.
Remark 22. The results in the work show that by means of appropriate impulsive perturbations, we can control the dynamics of these equations.
Acknowledgments
This work was supported by the Construct Program of the Key Discipline in Hunan Province. Research was supported by the National Natural Science Foundation of China (10971229, 11161015), the China Postdoctoral Science Foundation (2012M512162), and Hunan Provincial Natural Science-Hengyang United Foundation of China (11JJ9002).